• 제목/요약/키워드: $ReMnO_3$

검색결과 36건 처리시간 0.033초

Effect of Ce0.9Gd0.1O1.95 as a promoter upon the oxygen transfer properties of MgMnO3-δ-Ce0.9Gd0.1O1.95 composite oxygen carrier materials for chemical looping combustion

  • Hwang, Jong Ha;Lee, Ki-Tae
    • Journal of Ceramic Processing Research
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    • 제20권1호
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    • pp.18-23
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    • 2019
  • Chemical looping combustion (CLC) is a promising carbon capture and storage (CCS) technology whose efficiency and cost primarily relies on the oxygen carrier materials used. In this paper, gadolinium-doped ceria (GDC, Ce0.9Gd0.1O1.95) was added as a promoter to improve the oxygen transfer rate of MgMnO3-δ oxygen carrier materials. Increasing GDC content significantly increased the oxygen transfer rate of MgMnO3-δ-GDC composites for the reduction reaction due to an increase in the surface adsorption of CH4 via oxygen vacancies formed on the surface of the GDC. On the other hand, the oxygen transfer rate for the oxidation reaction decreased linearly with increasing GDC content due to the oxygen storage ability of GDC. Adsorbed oxygen molecules preferentially insert themselves into oxygen vacancies of the GDC lattice rather than reacting with (Mg,Mn)O to form MgMnO3-δ during the oxidation reaction.

졸-겔법에 의한 (YbxY1-x)MnO3강유전체 박막제조 (Preparation of Ferroelectric (YbxY1-x)MnO3 Thin Film by Sol-Gel Method)

  • 강승구;이기호
    • 한국세라믹학회지
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    • 제41권2호
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    • pp.170-175
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    • 2004
  • Y-acetate, Yb-acetate와 Mn-acetate를 출발물질로 사용하여 sol-gel 법으로 강유전성 (Y $b_{x}$ $Y_{1-x}$)Mn $O_3$ 박막을 제조하였다. Acetylaceton을 촉매로 사용하고 Reflux 법을 이용하여 안정한 (Y $b_{x}$ $Y_{1-x}$)Mn $O_3$ 전구체 용액을 얻었으며, 박막은 스핀 코팅방법으로 Si(100) 기판 위에 제조하였다 열처리 온도, 코팅용액의 Rw($H_2O$/alkoxide moi ratio)변화 등을 실험변수로 하여 박막의 결정상 변화를 연구하였다. X-선 회절분석 결과 YbMn $O_3$의 결정상을 얻기 위한 최저 열처리온도는 7$50^{\circ}C$이었으며, 최적 열처리 조건은 80$0^{\circ}C$였다 Rw를 1∼6 범위 내에서 조절하여 첨가한 결과, Rw=1의 조건에서 c-축 배향이 잘 발달된 hexagonal YbMn $O_3$ 단일 결정상을 얻었다. Si(100)기판 위에 제조된 (Y $b_{x}$ $Y_{1-x}$)Mn $O_3$ 박막은 x=0 또는 1인 경우 잔류분극(Pr)값이 약 200 nC/$ extrm{cm}^2$을 나타내었으나 0

$La_{0.7}Ca_{0.3-x}Ba_xMnO_3$ manganites : Local structure and transport properties

  • A.N.Ulyanov;Yang, Dong-Seok;Yu, Seong-Cho
    • 한국결정학회:학술대회논문집
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    • 한국결정학회 2003년도 춘계학술연구발표회
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    • pp.8-8
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    • 2003
  • Electron-phonon interaction plays a significant role in forming of colossal magnetoresistance effect (CMR). Polaron formation was observed by neutron diffraction and by extended X-ray absorption fine structure (EXAFS) analysis. Local probe as given by the EXAFS is a useful method to study the polaronic charge and its dependence on temperature and ions size. Here we present the EXAFS study of polaronic charge in La/sub 0.7/Ca/sub 0.3-X/Ba/sub X/MnO₃ compositions. The single phase La/sub 0.7/Ca/sub 0.3-X/Ba/sub X/MnO₃ manganites (x=0; 0.03; 0.06, ..., 0.3) were prepared by ceramic technology [1]. The Curie temperature was determined by extrapolation of the temperature dependence of the magnetization (down to zero magnetization). EXAFS experiments were carried out at the 7C EC beam line of the Pohang Light Source (PLS) in Korea. The atomic pair distribution functions (PDF) were obtained by re-regularization method [2] from filtered spectra. The PDF for the x=0.3 sample showed a single peak function and for x=0.0, 0.03, 0.06, 0.09, 0.12 compositions were asymmetric in agreement with a small Jahn-Teller elongation of two (short and long) bonds of the MnO/sub 6/ octahedron. Dispersion, σ/sub Min-O//sup 2/, and asymmetry, σ/sub Min-O//sup 3/, of the Mn-O bond distances varied significantly with x and showed a maximums at x=0.09. The maximum of σ/sub Min-O//sup 2/ is caused by increase of dynamic rms displacements of the Mn-O distances near the T/sub C/. The observed x dependence of σ/sub Min-O//sup 3/ reflects the reduction of charge carriers mobility at approaching to T/sub C/ from low as well as high temperatures.

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실험계획법을 적용한 X7R 적층 칩 커패시터의 희토류(Y2O3, Er2O3) 첨가에 따른 전기적 특성 (The Electrical Properties of Mutilayer Chip Capacitor with X7R by Addition of Rare-Earth Ions (Y2O3, Er2O3) using Design of Experiments)

  • 윤중락;문환;이헌용
    • 한국전기전자재료학회논문지
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    • 제23권3호
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    • pp.216-221
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    • 2010
  • Employing statistical design of experiments, the difference in doping behaviors of rare-earth ions and their effects on the dielectric property and microstructure of $BaTiO_3$-MgO-$MnO_2$-($Ba_{0.4}Ca_{0.6}$) $SiO_3-Re_2O_3$ (Re = $Y_2O_3$, $Er_2O_3$) system were investigated. Through the statistical analysis we have found that the amount of $Re_2O_3$ are significantly affecting on the dielectric properties. The $Re_2O_3$ improved the dielectric constant, dielectric loss and R*C constant, so the appropriate contents of $Y_2O_3$ and $Er_2O_3$ were 0.8 ~ 1.2 mol% and 0.8 ~ 1.3 mol%, respectively. The MLCC(mutilayer chip capacitor) with $2.0{\times}1.2{\times}1.2mm$ size and 475 nF was also suited for X7R with the above composition. It showed that the dielectric constant and RC constant were 2,839 and 3,675 ${\Omega}F$, respectively in the sintering condition at $1250^{\circ}C$ in $Po_2$ $10^{-7}$ Mpa.

박막형 고온초전도 선재를 위한 산화물 완충층의 IBAD_MgO 기판에서의 성장과 특성 (Growth and characterization of oxide buffer layer on IBAD_MgO template for HTS coated conductors)

  • 고락길;장세훈;하홍수;김호섭;송규정;하동우;오상수;박찬;문승현;김영철
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2008년도 하계학술대회 논문집 Vol.9
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    • pp.297-297
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    • 2008
  • Buffer layers play an important role in the development of high critical current density coated conductor. $LaMnO_3$, $SrTiO_3$ and $BaZrO_3$ buffer layers were compatible with MgO surfaces and also provide a good template for growing high current density REBCO(RE=Rare earth) films. Systematic studies on the influences of pulsed laser deposition parameters (deposition temperature, deposition pressure, processing gas, laser energy density, etc.) on microstructure and texture properties of $LaMnO_3$, $SrTiO_3$ and $BaZrO_3$ films as buffer layer deposited on ion-beam assisted deposition MgO (IBAD_MgO) template by pulse laser deposition method, were carried out. These results will be presented together with the discussion on the possible use of this material in HTS coated conductor as buffer.

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EPR SPECTRA OF Mn ION WITH TWO PHASES IN THE Y-Ba-Cu-Mn-O HIGH Tc SUPERCONDUCTOR

  • Kim, Seon-Ok;Rudowicz, Czeslaw;Lee, Soo-Hyung;Yu, Seong-Cho
    • 한국자기학회지
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    • 제5권5호
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    • pp.782-785
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    • 1995
  • In this paper, $Mn^{2+}$ ion was doped in Y-Ba-Cu-O as an EPR probe. The following samples were prepared by conventional solid-state reaction method : $YBa_{2}Cu_{2.96}Mn_{0.04}O_{7-\delta}$ (MN-I), annealed $YBa_{2}Cu_{2.96}Mn_{0.04}O_{7-\delta}$ (AMN) and $YBa_{2}Cu_{2.94}Mn_{0.06}O_{7-\delta}$ (MN-II). AMN sample was obtained from MN-I by annealing for 1 hr under the Ar gas atmosphere at $600^{\circ}C$. X-band (~9.05 GHz) EPR spectra were measured from 103 K to room temperature by employing a JES-RE3X spectroscopy with a $TE_{0.11}$ cylindrical cavity and 100 kHz modulation frequency. In MN-I we have observed only the $Cu^{2+}$ signal. The fact that no $Mn^{2+}$ signal was observed, in spite of $Mn^{2+}$ being a very sensitive EPR probe, indicates that most likely isolated $Mn^{2+}$ ions don't exist in the MN-I sample. Most probably $Mn^{2+}$ ions in the MN-I sample interact antiferromagnetically and hence are EPR silent. The AMN spectra of at room temperature and 103 K indicate not only the $Cu^{2+}$ signal but also an extra signal, which increases with decreasing temperature. It is suggested that the extra signal originates from Mn ions that were antiferromagnetically coupled before the annealing process. In MN-II, from 103 K to room temperature, also, the extra signal was observed together with the $Cu^{2+}$ signal. The extra signal in MN-II, however, decreases with decreasing temperature and nearly disappears at 103 K. The signal originates from Mn ions in impurity phases that include $Mn^{2+}$ ions. We suppose that there exist at least two $Mn^{2+}$ doped phases in Y-Ba-Cu-O. The $Mn^{2+}$ signal of one phase is undectable at all temperature and that of another phase decreases with decreasing temperature and disappears around 103 K.

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Electrical and Magnetic Properties in [La0.7(Ca1-xSrx)0.3MnO3)]0.99/(BaTiO3)0.01 Composites

  • Kim, Geun-Woo;Bian, Jin-Long;Seo, Yong-Jun;Koo, Bon-Heun
    • 한국재료학회지
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    • 제21권4호
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    • pp.216-219
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    • 2011
  • Perovskite manganites such as $RE_{1-x}A_xMnO_3$ (RE = rare earth, A = Ca, Sr, Ba) have been the subject of intense research in the last few years, ever since the discovery that these systems demonstrate colossal magnetoresistance (CMR). The CMR is usually explained with the double-exchange (DE) mechanism, and CMR materials have potential applications for magnetic switching, recording devices, and more. However, the intrinsic CMR effect is usually found under the conditions of a magnetic field of several Teslas and a narrow temperature range near the Curie temperature ($T_c$). This magnetic field and temperature range make practical applications impossible. Recently, another type of MR, called the low-field magnetoresistance(LFMR), has also been a research focus. This MR is typically found in polycrystalline half-metallic ferromagnets, and is associated with the spin-dependent charge transport across grain boundaries. Composites with compositions $La_{0.7}(Ca_{1-x}Sr_x)_{0.3}MnO_3)]_{0.99}/(BaTiO_3)_{0.01}$ $[(LCSMO)_{0.99}/(BTO)_{0.01}]$were prepared with different Sr doping levels x by a standard ceramic technique, and their electrical transport and magnetoresistance (MR) properties were investigated. The structure and morphology of the composites were studied by X-ray diffraction (XRD) and scanning electronic microscopy (SEM). BTO peaks could not be found in the XRD pattern because the amount of BTO in the composites was too small. As the content of x decreased, the crystal structure changed from orthorhombic to rhombohedral. This change can be explained by the fact that the crystal structure of pure LCMO is orthorhombic and the crystal structure of pure LSMO is rhombohedral. The SEM results indicate that LCSMO and BTO coexist in the composites and BTO mostly segregates at the grain boundaries of LCSMO, which are in accordance with the results of the magnetic measurements. The resistivity of all the composites was measured in the range of 90-400K at 0T, 0.5T magnetic field. The result indicates that the MR of the composites increases systematically as the Ca concentration increases, although the transition temperature $T_c$ shifts to a lower range.

Ce가 첨가된 Mn-Ce/${\gamma}-Al_2O_3$ 촉매상에서 톨루엔의 촉매 산화 반응 (Catalytic Oxidation of Toluene over Mn-Ce/${\gamma}-Al_2O_3$ Catalyst Doped with Ce)

  • 천태진;김혜진;최성우
    • 대한환경공학회지
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    • 제27권5호
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    • pp.513-518
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    • 2005
  • 망간 산화물 촉매, 망간-세륨 산화물 촉매에서 톨루엔의 촉매 산화에 대하여 조사 하였다. XRD, TGA, 톨루엔-TPR 분석을 통해 촉매의 특성을 조사하였다. 톨루엔 산화반응에 있어서 망간 18.2 wt.% 세륨 10.0 wt.%이 적절한 비율인 것으로 나타났다. 그리고 세리아가 망간 산화물에서의 활성을 증진 시키는 것으로 보여진다. XRD결과 $MnO_2$가 황성 자리인 것으로 추측된다. TGA 톨루엔-TPR결과 세리아가 격자 산소의 이동성, 활성자리의 적절한 상화 상태, 저온에서의 환원능력 및 활성자리의 재산화 능력을 증진시키는 것으로 사료된다.

고효율 압전 트랜스포머용 PSN-PMN-PZT 조성 설계 (Energy Efficient Alloy Design in PSN-PMN-PZT Ceramic System for Piezoelectric Transformer Application)

  • 최용길;어순철;윤만순
    • 한국재료학회지
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    • 제15권12호
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    • pp.814-817
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    • 2005
  • In order to enhance energy efficiency in high electric conversion devices such as Power transformers, which need to have high power properties, an alloy design approach in $Pb(Zr,Ti)O_3(PZT)$ base ceramic system was attempted $0.03Pb(Sb_{0.5}Nb_{0.5})O_3-0.03Pb(Mn_{1/3}Nb_{2/3})O_3-(0.94-x)PbTiO_3-xPbZrO_3$[PSN-PMN- PZT] ceramics were synthesized by conventional bulk ceramic processing technique. To improve power properties, the various Zr/Ti ratio was varied ]lear their morphotropic phase boundary (MPB) composition of PSN-PMN-PZT system and their effects on subsequent piezoelectric and dielectric properties for the transformer application at high power were systematically investigated using an impedance analyzer. Microstructure and phase information were characterized using X-ray diffractometer (XRD), a scanning electron microscope (SEM) and others. When the Zr/Ti ratio was 0.415/0.465, the value of $Q_m\;and\;k_p$ were shown to reach to the maximum, indicating that this alloy design can be a feasible composition :or high power transformer.